{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:U5VEWRZJJWDIHTJ6W57YBB45SU","short_pith_number":"pith:U5VEWRZJ","schema_version":"1.0","canonical_sha256":"a76a4b47294d8683cd3eb77f80879d9526428d632e9d04c408dca3a7dd9a945a","source":{"kind":"arxiv","id":"1004.0841","version":2},"attestation_state":"computed","paper":{"title":"Dilepton Signal of a Type-II Seesaw at CERN LHC: Reveals a TeV Scale B-L Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Narendra Sahu, Swarup Kumar Majee","submitted_at":"2010-04-06T12:50:54Z","abstract_excerpt":"We explore the discovery potential of doubly charged Higgs bosons (\\xi^{\\pm\\pm}) at the CERN Large Hadron Collider (LHC). For moderate values of the coupling constants in the original Type-II seesaw model, these doubly-charged Higgs bosons are not accessible by any present or near future collider experiments. In a gauged B-L symmetric model we introduce two triplet scalars to execute a variant of type-II seesaw at the TeV scale. This leads to a clear like-sign dilepton signal in the decay mode of \\xi^{\\pm\\pm} for a small vacuum expectation value (\\lsim 10^5 \\eV) of the triplet scalar \\xi= (\\xi"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1004.0841","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-06T12:50:54Z","cross_cats_sorted":[],"title_canon_sha256":"a6201da4125b3a48a4f555203f1ae885c00884055a8a4111defe75c89d32fb74","abstract_canon_sha256":"44abdef3738bcd5f215c15e60f715de38f3e49f6d9006fc3995426494fab33c0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:17.370338Z","signature_b64":"KX0uLtCua7Vdb0GhmA/eMrsSS9rpqOiKCA9ryIB4YiAIgeFPmHJiy+eYlgjC7Ue8NEcOM04KnU4VIs3nyz1/Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a76a4b47294d8683cd3eb77f80879d9526428d632e9d04c408dca3a7dd9a945a","last_reissued_at":"2026-05-18T02:24:17.369625Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:17.369625Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dilepton Signal of a Type-II Seesaw at CERN LHC: Reveals a TeV Scale B-L Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Narendra Sahu, Swarup Kumar Majee","submitted_at":"2010-04-06T12:50:54Z","abstract_excerpt":"We explore the discovery potential of doubly charged Higgs bosons (\\xi^{\\pm\\pm}) at the CERN Large Hadron Collider (LHC). For moderate values of the coupling constants in the original Type-II seesaw model, these doubly-charged Higgs bosons are not accessible by any present or near future collider experiments. In a gauged B-L symmetric model we introduce two triplet scalars to execute a variant of type-II seesaw at the TeV scale. This leads to a clear like-sign dilepton signal in the decay mode of \\xi^{\\pm\\pm} for a small vacuum expectation value (\\lsim 10^5 \\eV) of the triplet scalar \\xi= (\\xi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.0841","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1004.0841","created_at":"2026-05-18T02:24:17.369742+00:00"},{"alias_kind":"arxiv_version","alias_value":"1004.0841v2","created_at":"2026-05-18T02:24:17.369742+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.0841","created_at":"2026-05-18T02:24:17.369742+00:00"},{"alias_kind":"pith_short_12","alias_value":"U5VEWRZJJWDI","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"U5VEWRZJJWDIHTJ6","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"U5VEWRZJ","created_at":"2026-05-18T12:26:15.391820+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.23038","citing_title":"Mono-Z' Signatures in the B-L Supersymmetric Standard Model at the LHC","ref_index":6,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU","json":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU.json","graph_json":"https://pith.science/api/pith-number/U5VEWRZJJWDIHTJ6W57YBB45SU/graph.json","events_json":"https://pith.science/api/pith-number/U5VEWRZJJWDIHTJ6W57YBB45SU/events.json","paper":"https://pith.science/paper/U5VEWRZJ"},"agent_actions":{"view_html":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU","download_json":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU.json","view_paper":"https://pith.science/paper/U5VEWRZJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1004.0841&json=true","fetch_graph":"https://pith.science/api/pith-number/U5VEWRZJJWDIHTJ6W57YBB45SU/graph.json","fetch_events":"https://pith.science/api/pith-number/U5VEWRZJJWDIHTJ6W57YBB45SU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU/action/storage_attestation","attest_author":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU/action/author_attestation","sign_citation":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU/action/citation_signature","submit_replication":"https://pith.science/pith/U5VEWRZJJWDIHTJ6W57YBB45SU/action/replication_record"}},"created_at":"2026-05-18T02:24:17.369742+00:00","updated_at":"2026-05-18T02:24:17.369742+00:00"}